An excited-state atom whose emitted light is back-reflected by a distant mirror can experience trapping forces, because the presence of the mirror modifies both the electromagnetic vacuum field and the atom's own radiation reaction field. We demonstrate this mechanical action using a single trapped barium ion. We observe the trapping conditions to be notably altered when the distant mirror is shifted by an optical wavelength. The well-localised barium ion enables the spatial dependence of the forces to be measured explicitly. The experiment has implications for quantum information processing and may be regarded as the most elementary optical tweezers.PACS numbers: 42.50. Pq, 42.50.Vk, 32.80.Pj, 42.50.Ct An atom which sits in the vicinity of mirrors or reflectors experiences energy shifts of its electronic states. These level shifts are known as the van der Waals, Casimir-Polder [1] and resonant radiative shifts [2,3], the latter of which is caused by a retarded interaction of the atom with its own radiation field. For an atom in its excited state and at distances from a mirror much less than the transition wavelength, the level shift will be dominated by the van der Waals interaction, whilst in the far field the level shift is attributed to the resonant interaction with its own reflected field [3,4,5,6]. Such far-field shifts have been observed with an atomic beam traversing an optical resonator [7] and with atoms in a microwave cavity [8]. The same effect has been predicted for a single trapped ion whose emitted radiation field is reflected back by a single, distant mirror [9], and recently this level shift has been observed with an indirect spectroscopic method [10].The far-field mirror-induced shift of an excited atomic level oscillates on the wavelength scale when the atommirror distance is varied. Therefore, when the position of the atom is controlled to the extent that it becomes sensitive to this spatial dependence, then the level shift acts as a spatially varying potential U ( r), and the atom feels its gradient − ∇U ( r) as a force.This mirror-induced force is a peculiar manifestation of the mechanical effects of light. Forces due to applied light fields were first demonstrated experimentally by Lebedev [11], and the recoil of an absorbed photon on an atom was observed by Frisch who deflected an atomic beam with incoherent light [12]. With the advent of the laser, such forces have found many important applications, from decelerating, cooling and trapping atoms to optical tweezers in biology [13].Mirror-induced forces on individual atoms were first considered in connection with cavity-QED experiments, where their use has been proposed for trapping atoms in an optical resonator [14,15]. It is this kind of binding force which we observe in the experiment reported here. A single, trapped and laser-excited ion is an ideal system for this observation, as its position can be controlled on the nanometer scale [16,17,18], and interaction with a distant mirror has already been demonstrated [10,16,19]. These e...